Diode-pumped cavity

ABSTRACT

A side-pumped, diode-pumped solid-state laser cavity includes a conductively cooled housing having an opening O for pump radiation from a diode array in close proximity to a laser rod. The pump light is absorbed by the rod and excites the laser ions. The cavity includes a thin, diffuse reflector encircling the rod, having a shaped opening for the collection and redirection of the pump light into the rod, and a good heat conductor as the heat sink and heat conductor. A split heat sink inhibits the flow of heat from the pump diodes into the laser rod, and pre-formed air spacings are designed to provide uniform temperature distribution around the laser rod.

FIELD OF THE INVENTION

The present invention relates to side-pumped, diode-pumped solid-statelasers, and more particularly to a cavity for diode side pumping ofsolid-state laser rods as oscillators or amplifiers.

BACKGROUND OF THE INVENTION

Energetic diode-pumped lasers use laser diodes in various geometries,mostly arranged around the laser rod, performing side pumpingperpendicular to the rod axis. The light emitted by the laser diodesenters perpendicular to the rod axis. The pump light is absorbed by theatoms in the laser rod, exciting the atoms, thus establishing an opticalgain in the laser rod. The side pumping geometry allows a large excitedcross-section of the laser rod as well as long rod pumping, facilitatinglarge pumped volume and large energy storage and high-energy extractionas required.

The side-pumped, diode-pumped solid-state laser (side-pumped DPSSL)field can be divided into sub-fields based on how the otherwise highlydivergent, up to 40°, diode radiation is coupled into the laser rod.Some of these sub-fields include: (a) using optics such as a cylindricallens or elliptical mirror, (b) using an optical waveguide such as areflective cavity or fiber; and (c) closely coupling the diode(s) to therod.

The side-pumped, diode-pumped solid-state laser (side-pumped DPSSL)field can be farther divided into sub-fields based on how the heat,resulting from the method used to remove the part of the electric energyintroduced into the cavity that is not transferred to laser light isremoved. Some of these sub-fields include: (a) using liquid, circulatingin and out of the cavity, where the excessive heat is convected away,(b) using gas, circulating in and out of the cavity, where the excessiveheat is convected away, (c) using a solid-state structure, where theexcessive heat is conducted away through the solid structure. Heatremoval in most prior art arrangements and structures was performedusing compressed gas or liquid coolants. Gas or liquid coolants limitthe reliability of the laser system, since frequent preventivemaintenance activity is required to address leaks of the coolant ordegradation of its characteristics.

Japanese patent publication no. JP 5-259540 discloses a side-pumpedDPSSL wherein the rod is disposed within a diffuse reflector orcondenser. A diode array emits radiation that enters the condenser forabsorption by the rod via a narrow slit which guides the diode radiationtoward the rod. A gel or liquid such as water surrounds the rod fillingspacing between the rod and surrounding tube. Some light is absorbed inthe liquid, scattered and absorbed by multiple reflections.

U.S. Pat. Nos. 5,521,936, 5,033,058 and 6,026,109 disclose water-cooledsolid-state lasers using closely coupled side-pumping diode arrays. Thepumping laser diodes are disposed close to the rod in order that the rodremains in the path of the substantial portion of the divergentradiation, as it is not contemplated that rays missing the rod on thefirst pass will be subsequently redirected towards the rod to beabsorbed on a second or later pass, the efficiency is reduced. U.S. Pat.No. 5,870,421 patent differs in that it discloses the use ofside-pumping optical fibers, which add substantial manufacturing cost.

In addition, the alternative configurations described in U.S. Pat. Nos.5,521,936, 5,033,058 and 6,026,109 include a rod which is cooled with awater jacket enclosed a flow tube, with the diodes and reflectordisposed outside the flow tube, similarly to JP 5-259540. Here, adisadvantage is that the wall thickness of the flow tube addssignificant distance between the rod and reflector. In configurationsusing a diffuse reflector, this leads to increased losses of the pumplight, resulting in reduced efficiency.

U.S. Pat. No. 6,608,852 describes a liquid-cooled side-pumped laserincluding an elongated diffuse reflector housing having an elongatedcavity defined by a diffusely reflective cavity wall, with a solid-staterod disposed within the cavity and surrounded by a cooling fluid flowingalong the rod for cooling the rod. This laser has the advantage ofuniform pumping, but the liquid cooling is problematic in variousenvironmental conditions (like freezing).

In the close-coupled arrangement described in U.S. Pat. No. 5,774,488,the rod is enclosed in a heat-conducting specular reflector, and thepump radiation is introduced through a narrow slit in the reflector.This arrangement produces specular reflection, that causes non-uniformpumping of the rod cross section, and is complex to manufactures.Additionally, the specular reflector enhances the ASE (AmplifiedSpontaneous Emission) from the rod by providing parasitic laser paths.Additionally, any difference in thermal expansion of the rod andreflector may cause mechanical stress. Also, pump radiation from thediode must pass through a long narrow slit (channel) in the metalreflector, thus suffering multiple reflections and therefore extralosses.

Another problem is the type of reflector that can be used to pump light,while enabling uniform pumping of the rod cross section. Specularreflectors are not able to produce the same level of uniformity of thepump radiation as diffuse reflectors. For example, Hanson, et al.,citation below, disclose a three-bar diode array placed a small distanceaway from a large opening to a solid-state laser cavity. Ajer et al.,citation below, disclose a closely coupled side-pumping diode arraywhich pumps the rod through a slit-like opening. The cavities disclosedby Hanson, et al. and Ajer, et al. include highly reflective innersurfaces, and the intensity distributions of the pumping diode radiationwithin the rods lack homogeneity.

Generally, pumping with a diode array from one direction can lead to acylindrical intensity distribution (as shown, for example, in the paperby Hanson, et al.). This gives rise to a cylindrical thermal lens in therod, which, in turn, results in an astigmatic output beam of the laser.To improve circularity, some of the mentioned references describealternative arrangements which use pumping radiation from several (twoor more) directions. The problem with this approach, however, is thatlaser diodes tend to age differently, which destroys the intensitybalance over the lifetime of diodes.

In U.S. Pat. Nos. 5,317,585 and 5,781,580, a transparent heat conductoris used, since the heat conductor of these designs has to be opticallytransparent to allow the diode light to enter the laser rod and at thesame time conductively cool the rod. High optical transparency and highthermal conductivity properties are not readily found in one material(except in diamond which is extremely expensive and cannot be machinedto the needed shapes), and thus the solution is not optimized for any ofthe parameters.

Other references are:

Walter Koechner, “Solid-state Laser Engineering”, pp. 127-140, 709(Springer series in optical sciences, v.1, Springer-Verlag, Berlin,Heidelberg, New York, 1996).

Frank Hanson and Delmar Haddock, “Laser diode side pumping of neodymiumlaser rods”, Applied Optics, vol. 27, no. 1, 1988, pp. 80-83.

H. Ajer, et al., “Efficient diode-laser side-pumped TEM00-mode Nd:YAGlaser”, Optics Letters, vol. 17, no. 24, 1992, pp. 1785-1787.

Jeffrey J. Kasinski, et al., “One Joule Output From a Diode Array PumpedNd:YAG Laser with Side-pumped Rod Geometry”, J. of Quantum Electronics,Vol. 28, No. 4 (April 1992).

D. Golla, et al., “300-W cw Diode Laser Side-pumped Nd:YAG Rod Laser”,Optics Letters, Vol. 20, No. 10 (May 15, 1995).

Japanese Patent No. JP 5-259540.

U.S. Pat. Nos. 5,774,488, 5,521,936, 5,033,058, 6,026,109, 5,870,421,5,117,436, 5,572,541, 5,140,607, 4,945,544, 4,969,155, 5,875,206,5,590,147, 3,683,296, 3,684,980, 3,821,663, 5,084,886, 5,661,738,5,867,324, 5,963,363, 5,978,407, 5,661,738, 4,794,615, 5,623,510,5,623,510, 3,222,615, 3,140,451, 3,663,893, 4,756,002, 4,755,002,4,794,615, 4,872,177, 5,050,173, 5,317,585, 5,349,600, 5,455,838,5,488,626, 5,521,932, 5,590,147, 5,627,848, 5,627,850, 5,638,388,5,651,020, 5,838,712, 5,875,206, 5,677,920, 5,781,580, 5,905,745,5,909,306, 5,930,030, 5,987,049, 5,995,523, 6,009,114, and 6,002,695.

German Patent No. DE 689 15 421 T2.

Canadian Patent No. 1,303,198.

French Patents Nos. 1,379,289 and 2,592,530.

Fujikawa, et al., “High-Power High-Efficient Diode-Side-Pumped Nd: YAGLaser”, Trends in Optics and Photonics, TOPS Volume X, AdvancedSolid-state Lasers, Pollock and Bosenberg, eds., (Topical Meeting,Orlando, Fla., Jan. 27-29, 1997).

R. V. Pole, IBM Technical Disclosure Bulletin, “Active Optical ImagingSystem”, Vol. 7, No. 12 (May 1965).

Devlin, et al., “Composite Rod Optical Masers”, Applied Optics, Vol. 1,No. 1 (January 1962).

Goldberg et al., “V-groove side-pumped 1.5 um fibre amplifier,”Electronics Letters, Vol. 33, No. 25, Dec. 4, 1997).

Welford, et al., “Efficient TEM00-mode operation of a laser diodeside-pumped Nd:YAG laser, Optics Letters, Vol. 16, No. 23 (Dec. 1,1991).

Welford, et al., “Observation of Enhanced Thermal Lensing Due toNear-Gaussian Pump Energy Deposition in a Laser Diode Side-Pumped Nd:YAGLaser,” IEEE Journal of Quantum Electronics, Vol. 28, No. 4 (Apr. 4,1992).

Walker, et al., “Efficient continuous-wave TEM00 operation of atransversely diode-pumped Nd:YAG laser,” Optics Letters, Vol. 19, No. 14(Jul. 15, 1994).

Comaskey et al., “24-W average power at 0.537 um from an externallyfrequency-doubled Q-switched diode-pumped ND:YOS laser oscillator,”Applied Optics, Vol. 33, No. 27 (Sep. 20, 1994).

Novel solutions allowing efficient side pumping, uniform pumpdistribution across the rod, pumping with a single source and one sideand good conductive cooling are needed and are presented in thisinvention. The optimization of the mentioned parameters results insmaller volumes and weight as well.

SUMMARY OF THE INVENTION

It is therefore a broad object of the present invention to provide aside-pumped, diode-pumped solid-state laser cavity including aconductively cooled housing, having an opening for the pump radiationemerging from a diode array in close proximity and having a solid-state,diffuse reflector surrounding the laser rod. The pump light is absorbedby the rod and excites the laser ions. The pump-light that transversesthe rod without absorption is redirected into it by the diffusereflector.

It is a further object of the present invention to provide a side-pumpeddiode-pumped solid-state laser cavity where the rod is encircled by athin, diffuse reflector that functions to redirect the pump-light thattransverses the rod without absorption back into the rod. The reflectoralso has a shaped opening to redirect the pump light coming out at largeangle into the rod, and serves as a good heat conductor to the heatsink.

It is still a further object of the present invention to provide aside-pumped, diode-pumped solid-state laser cavity including a splitheat sink which significantly reduces the flow of heat from the pumpdiodes into the laser rod through either the diode itself or the commonheat sink.

It is still a further object of the present invention to provide aside-pumped, diode-pumped solid-state laser cavity including a thermoelectric cooler element as a conductive heat pump.

It is still a further object of the present invention to provide aside-pumped, diode-pumped solid-state laser cavity is including apre-formed air spacing designed to provide uniform temperaturedistribution around the laser rod.

It is still a further object of the present invention to provide a diodepumping cavity for a laser system which efficiently couples the diodelight into the laser rod directly, without using focusing lenses, prismsor windows, using only free air transmission and side redirection oflarge-angle pump beams.

It is still a farther object of the present invention to provide veryefficient conductive cooling of the laser rod. Conductive cooling iscarried out through a thin ceramic heat conductor, into a very goodmetallic heat conductor. The ceramic heat conductor is positionedopposite the diode array, and is also used as a light redirector. Theunabsorbed diode light is redirected by the ceramic material back intothe laser rod.

It is still a farther object of the present invention to provideenhancement of the radially symmetrical heat dissipation from the laserrod by adjusting the shape of the thermal conductor and using machinedair spacings to control heat conduction.

It is still a further object of the present invention to provide opticalproximity between pump diodes and a laser rod while maintaining thermalisolation, since most of the heat (about 50% of the input energy) isdissipated in the pump diode stack, and only a small portion in the rod(about 10% of the input energy).

A side-pumped, diode-pumped solid-state laser cavity is providedincluding a conductively cooled housing having an opening for pumpradiation from a diode array in close proximity to a laser rod. The pumplight is absorbed by the rod and excites the laser ions. The cavityincludes a thin, diffuse reflector encircling the rod, having a shapedopening for the collection and redirection of the pump light into therod, and a good heat conductor as the heat sink and heat conductor.

The cavity can also include a split heat sink that inhibits the flow ofheat from the pump diodes into the laser rod, and pre-formed airspacings designed to provide uniform temperature distribution around thelaser rod.

In one embodiment, a side-pumped diode-pumped solid-state laser cavityincludes a conductively cooled housing, having a solid-state, diffusereflector surrounding the laser rod. The pump light passes through anopening in the diffuse reflector, into the rod in close proximity, andis absorbed by the rod and excites the laser ions. The pump-light thattransverses the rod without absorption is redirected into the rod by thediffuse reflector.

The laser rod is preferably conductively cooled. The reflector ispreferably of diffuse type and placed as close to the rod as possible.The pump radiation preferably comes from one source, but still producesa circularly symmetrical intensity distribution inside the rod.

The higher the optical pumping efficiency of the laser rod, the less thethermal loading of the laser rod, resulting in a higher optical qualityof the rod and a better output beam quality. In addition,high-efficiency pumping reduces the number of diode arrays required toobtain a specified laser energy output, reducing further the size andthe cost of the laser system. Smaller size, less input power and betterlaser output quality can be achieved.

High pumping efficiency is achieved by good optical coupling of thediode light into the laser rod and adequate absorption of the diodelight in the laser rod. The angular divergence of the diode light in thetransverse plane is about 40°, and thus, a substantial fraction of thelight will miss the laser rod. In addition, another fraction of thelight will be lost due to Fresnel reflections caused by the high indexof refraction and small diameter of the laser rod. Any focusing lenseswhich can be used to focus the diode light into the laser rod will causelight losses, due to limited lens aperture and optical lens coatings.For example, in U.S. Pat. Nos. 4,755,002 and 4,969,155, due to thementioned problems of coupling linear diode arrays into the laser rod,focusing lenses were utilized perceptively, reducing the opticalcoupling efficiency.

BRIEF DESCRIPTION OF THE DRAWINGS

The invention will now be described in connection with certain preferredembodiments and with reference to the following illustrative figures sothat it may be more fully understood. The particulars shown are by wayof example and for purposes of illustrative discussion of the preferredembodiments of the present invention only, and are presented in thecause of providing what is believed to be the most useful and readilyunderstood description of the principles and conceptual aspects of theinvention. In this regard, no attempt is made to show structural detailsof the invention in more detail than is necessary for a fundamentalunderstanding of the invention, the description taken with the drawingsmaking apparent to those skilled in the art how the several forms of theinvention may be embodied in practice.

In the drawings:

FIG. 1 is a schematic, cross-sectional view of a side-pumped,diode-pumped solid-state laser cavity.

FIG. 2 is a schematic, cross-sectional view of the rod surroundings inthe side-pumped diode-pumped, solid-state laser cavity

FIG. 3 is a schematic, cross-sectional view of the rod surroundings ofthe side-pumped diode-pumped solid-state laser cavity with emphasis onthe entrance reflector.

DETAILED DESCRIPTION OF PREFERRED EMBODIMENTS

Referring now to FIG. 1, there is shown a schematic, cross-sectionalview of a side-pumped, diode-pumped solid-state laser cavity. A diodelaser stack 2 embedded in a heat-conducting cladding 4 emits pump lightthrough a lower opening 6 into a laser rod 8, which can be, e.g., Nd:YAGor any other solid-state crystal-doped with rare earth ions. The rareearth ions, e.g., Nd, are excited by the pump light and emit theirtypical radiation when needed. The laser rod 8 is surrounded by aceramic diffuse reflector 10 having three roles. The first role isredirecting the pump light photons that pass through the laser rod 8without being absorbed, or miss the rod geometrically. These photons areredirected in a diffuse way and go back and forth until absorbed in therod 8. Regular ceramics like alumina (Al oxide) or Zr oxide have veryhigh reflection coefficients, (higher than metal coatings such as goldor silver) and are very efficient in preserving the photons inside therod volume. The second role of the ceramic diffuse reflector 10 is toconduct the heat dissipated into the rod 8 by the pump light 2 into aheat sink part 12, through which the heat is carried out to the externalenvironment 14 via thermo electric cooler (TEC), 16. This heatconduction is performed through a short distance of ceramic in thereflector 10 (e.g., 0.2 to 1 mm of alumina) and a longer path (e.g., 10to 15 mm) in the heat sink 12, which can be made of a material (e.g.,copper), having much higher thermal conductively than alumina. The thirdrole of the ceramic diffuse reflector 10 is to redirect light from thestack 2 into the rod 8, as depicted in detail in FIG. 2. Between thediode cladding 4 and the TEC 16 is a copper or good heat-conductingspacer 18 formed as part of the combined rod-pump heat sink. The space18 keeps the mechanical assembly rigid and isolates thermally the diodepart, where it provides good optical proximity between the pump diodes 2and the laser rod 8 while maintaining thermal isolation through a small(few hundred micrometers) spacing or gap 20. This isolation is desirablesince most of the heat (about 50% of the input energy) is dissipated inthe pump diode stack 2, and only a small portion in the rod 8 (about 10%of the input energy).

In FIG. 2, there is shown a schematic, cross-sectional view of the rodsurroundings of the side-pumped diode-pumped, solid-state laser cavity.Here the light rays 26 leaving the lower exit of the diode stack 2 inlarge angle (which can be up to 40°) are redirected when impinging onthe outer slit 22 of the ceramic diffuse reflector 10. The redirectionis carried out by diffuse reflection at 22. Recalling that the thicknessof the ceramic diffuse reflector 10 is 0.2 to 1 mm, the amount of lightimpinging on 22 is small. The gap 28 is empty (e.g., air, nitrogen orvacuum), and thus does not interfere in the optical path, needs nolenses or prisms for redirection and provides a good thermal barrierbecause only line edges of the ceramic diffuse reflector 10 touch thecladding 4, as depicted in FIG. 2. Further tailoring of the temperatureprofile around the rod 8 is done by cutting (e.g. using wire sparkerosion techniques) lines 24, straight or curved, according to heat flowsimulations of the heat sink 12 and the rod 8 as a heat source.

FIG. 3 is a schematic, cross-sectional view of the rod surroundings ofthe side-pumped diode-pumped solid-state laser cavity with a modifiedentrance reflector. Here the angle 30 is designed to accommodate thelarge angle output of the diode, at its external part, leading it mostlyinto the rod 8 using diffuse reflection of the area 22. The angle 30 ispreferably less than the divergence angle of the diodes in the air space28.

It will be evident to those skilled in the art that the invention is notlimited to the details of the foregoing described and illustratedembodiments and that the present invention may be embodied in otherspecific forms without departing from the spirit or essential attributesthereof. The present embodiments are therefore to be considered in allrespects as illustrative and not restrictive, the scope of the inventionbeing indicated by the appended claims rather than by the foregoingdescription, and all changes, which come within the meaning and range ofequivalency of the claims, are therefore intended to be embracedtherein.

1. A side-pumped, diode-pumped solid-state laser cavity comprising atleast one pump laser diode, a laser rod, a conductively cooled housing,having an opening for pump radiation from said pump laser diode, and asolid-state, diffuse reflector surrounding the laser rod.
 2. Aside-pumped diode-pumped solid-state laser cavity as in claim 1, wherethe rod is encircled by a thin, diffuse reflector for redirecting thepump-light that transverses the rod without absorption back into therod, redirecting the pump light coming out of the pump laser diode at alarge angle into the rod, and serving as a good heat conductor to a heatsink.
 3. A side-pumped, diode-pumped solid-state laser cavity as inclaim 1, including a split heat sink which inhibits the flow of heatfrom the pump laser diode into the laser rod.
 4. A side-pumped,diode-pumped solid-state laser cavity as in claim 1, including a thermoelectric cooler element as a conductive heat pump.
 5. A side-pumped,diode-pumped solid-state laser cavity as in claim 1, including apre-formed empty space designed to provide uniform temperaturedistribution around the laser rod.
 6. A side-pumped, diode-pumpedsolid-state laser cavity as in claim 1, where efficient coupling oflight from the pump laser diode into the laser rod is done directly,without using focusing lenses, prisms or windows, using only free spacetransmission and side, angled, diffuse or specular, redirection of largeangle pump beams. 7 A side-pumped diode-pumped solid-state laser cavityas in claim 1, where very efficient conductive cooling is carried outthrough a thin ceramic thermal conductor, into a metallic heatconductor.
 8. A side-pumped, diode-pumped solid-state laser cavity as inclaim 7, where enhancement of the radially symmetrical heat dissipationfrom the laser rod is done by adjusting the shape of the thermalconductor and using machined air spacings to control heat conduction. 9.A side-pumped diode-pumped solid-state laser cavity as in claim 1,having optical proximity between pump diodes and laser rod whilemaintaining thermal isolation.
 10. A method for diode side pumping ofsolid-state laser rods, comprising side pumping light from at least onepump laser diode into a laser rod, and redirecting pump-light thattraverses said rod without absorption back into said rod with a diffusereflector
 11. The method of claim 10 which includes redirecting the pumplight coming out of the pump laser diode at a large angle into the rod.12. The method of claim 10 which includes inhibiting the flow of heatfrom the pump laser diode into the laser rod.
 13. The method of claim 10which includes a thermo electric cooler element as a conductive heatpump.
 14. The method of claim 10 which includes providing uniformtemperature distribution around the laser rod.
 15. The method of claim10 wherein efficient coupling of light from the pump laser diode intothe laser rod is done directly, without using focusing lenses, prisms orwindows, using only free space transmission and side, angled, diffuse orspecular, redirection of large angle pump beams. 16 The method of claim10 which includes conductive cooling carried out through a thin ceramicthermal conductor, into a metallic heat conductor.
 17. The method ofclaim 16 which includes adjusting the shape of the thermal conductor toenhance the radially symmetrical heat dissipation from the laser rod.18. The method of claim 10 which includes having optical proximitybetween pump diodes and laser rod while maintaining thermal isolation.